<p>We consider the following stationary FitzHugh-Nagumo system: <Equation ID="Equ61"> <EquationSource Format="TEX">\( \left\{ \begin{aligned}&amp;-\varepsilon ^2\Delta U =f(U)- V, \qquad&amp;\text {in}\ \Omega ,\\&amp;-\Delta V+\gamma V =\delta _\varepsilon U,&amp;\text{ in }\ \Omega ,\\&amp;U = V =0,&amp;\text {on}\ \partial \Omega , \end{aligned} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <msup> <mi>ε</mi> <mn>2</mn> </msup> <mi mathvariant="normal">Δ</mi> <mi>U</mi> <mo>=</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>U</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>V</mi> <mo>,</mo> <mspace width="2em" /> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>V</mi> <mo>+</mo> <mi>γ</mi> <mi>V</mi> <mo>=</mo> <msub> <mi>δ</mi> <mi>ε</mi> </msub> <mi>U</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow /> </mtd> <mtd columnalign="left"> <mrow> <mi>U</mi> <mo>=</mo> <mi>V</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <mrow> <mtext>on</mtext> <mspace width="4pt" /> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is a smooth bounded domain in <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\delta _{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>δ</mi> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> are positive parameters. The nonlinear term <i>f</i>(<i>U</i>) is given by <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(U(U-a)(1-U)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>U</mi> <mo stretchy="false">(</mo> <mi>U</mi> <mo>-</mo> <mi>a</mi> <mo stretchy="false">)</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>U</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, where <i>a</i>(<i>x</i>) is a smooth positive function in <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(C^2(\Omega )\cap C^1(\overline{\Omega })\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>C</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> <mo>∩</mo> <msup> <mi>C</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mover> <mi mathvariant="normal">Ω</mi> <mo>¯</mo> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with values in <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\((0,\frac{1}{2})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Using the Lyapunov–Schmidt reduction method, we rigorously establish the existence of multi-peaked solutions. Each peak is shown to concentrate near a nondegenerate critical point of the inhomogeneity <i>a</i>(<i>x</i>). Furthermore, we analyze the spectrum of the associated linearized operator. The large eigenvalues(of order O(1)) analysis shows that the constructed multi-peaked solution is linearly unstable. For the small eigenvalues(of order o(1)), we prove that they are of order <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(O(\varepsilon ^2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <mo stretchy="false">(</mo> <msup> <mi>ε</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, and their rescaled accumulation points are characterized by a finite-dimensional eigenvalue problem involving the Hessian matrices of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(a(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> at the concentration points.</p>

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Existence and stability analysis of multi-peaked solution for the FitzHugh-Nagumo system in \(\mathbb {R}^2\)

  • Jiaming Jin,
  • Bingqi Wang,
  • Xiangyu Zhou

摘要

We consider the following stationary FitzHugh-Nagumo system: \( \left\{ \begin{aligned}&-\varepsilon ^2\Delta U =f(U)- V, \qquad&\text {in}\ \Omega ,\\&-\Delta V+\gamma V =\delta _\varepsilon U,&\text{ in }\ \Omega ,\\&U = V =0,&\text {on}\ \partial \Omega , \end{aligned} \right. \) - ε 2 Δ U = f ( U ) - V , in Ω , - Δ V + γ V = δ ε U , in Ω , U = V = 0 , on Ω , where \(\Omega \) Ω is a smooth bounded domain in \(\mathbb {R}^2\) R 2 , and \(\varepsilon \) ε , \(\gamma \) γ , and \(\delta _{\varepsilon }\) δ ε are positive parameters. The nonlinear term f(U) is given by \(U(U-a)(1-U)\) U ( U - a ) ( 1 - U ) , where a(x) is a smooth positive function in \(C^2(\Omega )\cap C^1(\overline{\Omega })\) C 2 ( Ω ) C 1 ( Ω ¯ ) with values in \((0,\frac{1}{2})\) ( 0 , 1 2 ) . Using the Lyapunov–Schmidt reduction method, we rigorously establish the existence of multi-peaked solutions. Each peak is shown to concentrate near a nondegenerate critical point of the inhomogeneity a(x). Furthermore, we analyze the spectrum of the associated linearized operator. The large eigenvalues(of order O(1)) analysis shows that the constructed multi-peaked solution is linearly unstable. For the small eigenvalues(of order o(1)), we prove that they are of order \(O(\varepsilon ^2)\) O ( ε 2 ) , and their rescaled accumulation points are characterized by a finite-dimensional eigenvalue problem involving the Hessian matrices of \(a(x)\) a ( x ) at the concentration points.